Apply Snell geometry without inventing impossible rays
Body-wave paths bend when wave speed changes. For a plane isotropic interface, the ratio sin(angle from normal)/speed is conserved across a transmitted ray. A faster lower layer therefore bends the ray away from the normal, not toward it. Angles measured from the horizontal interface would use a different geometric expression.
Learning outcome: Change incidence across the critical threshold and retain the sine test before attempting an inverse sine. Sketch both directions and the interface normal. Record the no-propagating-ray condition rather than filling it with a fabricated angle.
Starting recap
Keep reference frames, material properties, path geometry and actual catalog evidence distinct. Infer only what the retained observations and stated model support.
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At incidence 30° and lower speed 8 km/s, sin r=2/3, so r≈41.8103°. The critical incidence is arcsin(6/8)≈48.5904°. A 60° incident ray would require a sine greater than one.
Open the experimentPredict
At a faster lower layer, does the transmitted angle become larger or smaller relative to the normal?
Experiment
Change incidence across the critical threshold and retain the sine test before attempting an inverse sine. Sketch both directions and the interface normal. Record the no-propagating-ray condition rather than filling it with a fabricated angle.
Trace a transmitted ray and its critical-angle limit
Worked teaching model · synthetic values · Plane isotropic interface; upper P speed 6 km/s, lower b≥6. Snell sin(i)/6=sin(r)/b. If sin(r)>1, no propagating transmitted body ray of this simple type; critical refraction and evanescent fields need fuller theory. Angles measured from normal, not interface.
Reset keeps your prediction, captures and practice history.
A faster lower layer bends a transmitted ray away from the normal until the critical limit.
No real refraction angle exists when the required sine exceeds one. This absence is a model condition, not permission to clamp the angle silently or conclude no seismic energy can travel along the interface.
| Quantity | Value | Unit |
|---|---|---|
| Incidence angle | 30 | degrees from normal |
| Snell transmitted sine | 0.66666667 | ratio |
| Critical angle | 48.590378 | degrees from normal |
| Propagating transmitted body ray admitted | 1 | 0 no / 1 yes |
| Refraction angle | 41.810315 | degrees from normal |
A faster lower layer bends a transmitted ray away from the normal until the critical limit.
No real refraction angle exists when the required sine exceeds one. This absence is a model condition, not permission to clamp the angle silently or conclude no seismic energy can travel along the interface.
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For incidence 60° and lower speed 10 km/s, is a propagating transmitted body ray admitted by this model?
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